bbq2014 said:
Hi jbriggs Could you elaborate more into why it can never be equal?
The differential equation of motion would be v'(x) = g - kv(x). If you are able to solve differential equations, this is an easy one and the solution involves an exponential.
Looking at it from a more simplistic viewpoint, suppose that you jump out of a hot air baloon. You are falling at 0 mph. Your terminal velocity is (let's say) 100 mph.
You fall for one second against negligible wind resistance, gaining roughly 20 mph. Now wind resistance is equal to about 20% of gravity.
You fall for another second against this wind resistance. This time you gain only 80% of 20 mph. That's another 16 mph for a total of 36 mph. Now wind resistance is equal to 36% of gravity.
You fall for another second against this wind resistance. This time you gain only 64% of 20 mph. That's another 12.8 mph for a total of 48.8 mph. Call it 50 mph. Now wind resistance is equal to 50% of gravity.
The closer your speed gets to terminal velocity the slower your speed increases. It never quite gets there. The difference decays geometrically. It took you three seconds to go from a 100 mph delta to a 50 mph delta. It will take another three seconds to get to a 25 mph delta. Another three to get to a 12.5 mph delta. Another three to get to a 6.25 mph delta.
So after 12 seconds, you're roughly at 95% of terminal velocity.
[The difference between the simplistic picture and the differential equation is that the differential equation is the ideal limit as one does the simplistic calculation using smaller and smaller time intervals]
What if you could scale this scenario up, let say you dropped it from the edge of the atmosphere? Is it due to the changing air density at different altitudes which changes the drag?
If you factor in the changes in air density, then "terminal velocity" starts out quite high at the edge of the atmosphere and reduces to more normal values as one descends. So a falling astronaut will fall at a high rate of speed initially (greater than the speed of sound). As he falls into denser air the corresponding terminal velocity will be decreasing. He will eventually be going faster than the [reduced] terminal velocity and will be slowing down rather than speeding up.